A catadioptric optical system comprising a first imaging optical system including a concave mirror and forming an intermediate image of a first object, said first imaging optical system forming a reciprocating optical system that an incidence light and reflected light pass, a second imaging optical system for forming an image of the intermediate image onto a second object, and a first optical path deflective member, provided between the concave mirror and the intermediate image, for introducing a light from the first imaging optical system to the second imaging optical system, wherein said first optical path deflective member deflects a light in such a direction that a forward path of the first imaging optical system intersects a return path of the first imaging optical system, and wherein said intermediate image is formed without an optical element after a deflection.
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1. A catadioptric optical system comprising:
a first imaging optical system including a concave mirror and forming an intermediate image of a first object, said first imaging optical system forming a reciprocating optical system that an incidence light and reflected light pass;
a second imaging optical system for forming an image of the intermediate image onto a second object;
a first optical path deflective member, provided between the concave mirror and the intermediate image, for introducing a light from the first imaging optical system to the second imaging optical system;
a second optical path deflective member provided between the intermediate image and the second object;
a lens unit, provided between the intermediate image and the second optical path deflective member,
wherein said first optical path deflective member deflects a light in such a direction that a forward path of the first imaging optical system intersects a return path of the first imaging optical system,
wherein said intermediate image is formed without an optical element after a deflection, and
wherein 6.80<|β1·βf/NAO|<10.60, is met, where β1 is a paraxial imaging magnification of the first imaging optical system, NAO is a numerical aperture of the light at the first object side, and βf is a paraxial imaging magnification of the lens unit.
2. A catadioptric projection optical system according to
3. A catadioptric projection optical system according to
4. A catadioptric projection optical system according to
5. A device fabrication method comprising the steps of:
exposing an object using an exposure apparatus according to
performing a development process for the object exposed.
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The present invention relates generally to a projection optical system, and more particularly to a catadioptric projection optical system that projects an object, such as a single crystal substrate and a glass plate for a liquid crystal display (“LCD”), using a mirror. The present invention is suitable, for example, an immersion exposure apparatus (an immersion lithography exposure system) for exposing the object through a fluid between the projection optical system and the object.
The photolithography technology for manufacturing fine semiconductor devices, such as semiconductor memory and logic circuits, has conventionally employed a reduction projection exposure apparatus that uses a projection optical system to project a circuit pattern of a reticle (or mask) onto a wafer, etc. A more highly integrated and finer semiconductor device (circuit pattern) requires a projection optical system for a better specification and performance. Generally, a shorter wavelength of the exposure light and a higher numerical aperture (“NA”) are effective to improve the resolution. Recently, an optical system with an NA of 1 or higher that utilizes an immersion optical system that fills a space with fluid between a final glass surface (in other words, the lens closet to the wafer) of the projection optical system and the wafer has been proposed, and a higher NA scheme is in progress.
For the exposure light with a short wavelength such as an ArF excimer laser (with a wavelength of approximately 193 nm) and a F2 laser (with a wavelength of approximately 157 nm) for higher resolution, lens materials are limited to quartz and calcium fluoride for reduced transmittance. An optical system that includes only lenses (refracting element) absorbs the large amount of light, and reduces an exposure dose on the wafer, causing a decrease in through put. Moreover, lens's heat absorption and resultant temperature rise disadvantageously fluctuate a focal position, (heat) aberrations, etc. Quartz and calcium fluoride possess similar dispersive powers, and have difficulties in correcting the chromatic aberration. Especially, the lens material can use only calcium fluoride for the exposure wavelength of 157 nm, and correcting the chromatic aberration becomes more difficult. In addition, a lens diameter increases as the NA becomes higher, and causes the increased apparatus cost.
Various proposals that use a mirror (reflecting element) for an optical system have been made to solve the disadvantageous reduced transmittance, difficult corrections to the chromatic aberration and large aperture of the lens. For example, a catadioptric projection optical system that combines a mirror with a lens has been disclosed. See, for example, U.S. Pat. No. 5,650,877 (reference 1), Japanese Patent Applications, Publication Nos. 62-210415 (reference 2), 62-258414 (reference 3), 5-188298 (reference 4), 6-230287 (reference 5), 2-66510 (reference 6), 3-282527 (reference 7), 8-304705 (reference 8), 2000-47114 (reference 9), and 2003-43362 (reference 10).
A projection optical system that includes a reflective optical system for a shorter exposure wavelength and a higher NA needs to correct the chromatic aberration, to maintain a large enough imaging area on an image surface, and to secure a sufficient working distance on the image side with a simple structure. The large enough imaging area on the image surface is advantageous to a scanning exposure apparatus to maintain the throughput, and reduce exposure fluctuations. The sufficient image-side working distance is desirable for an apparatus's auto-focusing system, a wafer-stage's transport system, and the like. The simple structure would simplify a barrel and the like, and facilitate the assembly production.
The optical system disclosed in the reference 1 arranges a Mangin mirror and a refractor in an optical system, and exposes a reticle image onto a wafer. Disadvantageously, this optical system blocks light on a pupil's central part for all the angles of view to be used (hollow illumination), and cannot enlarge an exposure area. An attempt to enlarge the exposure area results in the undesirable expansion of the light blockage on the pupil's central part. In addition, since a refractive surface of the Mangin mirror forms the light splitting surface that halves the light intensity when ever the light passes through its surface, and reduces the light intensity down to about 10% on the image surface (wafer surface).
The references 2 and 3 apply Cassegrain and Schwarzschild mirror systems, and each propose an optical system that has an opening at the center of the mirror to create a hollow illumination to the pupil and to image only the pupil's periphery. However, the hollow illumination on the pupil deteriorates the imaging performance. An attempt to lessen the hollow illumination to the pupil inevitably increases the power of the mirror and enlarges an angle incident upon the mirror. A high NA causes a mirror's diameter to grow remarkably.
According to the optical system disclosed in the references 4 and 5, the deflected optical path complicates an apparatus's configuration. A high NA is structurally difficult because the concave mirror is responsible for most powers in the optical units for imaging an intermediate image onto a final image. Since a lens system located between the concave mirror and the image surface is a reduction system and the magnification has a positive sign, the image-side working distance cannot be sufficiently secured. Since an optical path needs to be split, it is structurally difficult to secure an imaging area width. The large optical system is not suitable for foot-printing.
The references 6 and 7 first split an optical path using by the beam-splitter, and complicate the structure of a lens barrel. They need the beam-splitter with a large diameter and if the beam-splitter is a prism type, a loss of the light intensity is large due to its thickness. A higher NA needs a larger diameter and increases a loss of the light intensity. Use of a flat-plate beam splitter is also problematic, because it causes astigmatism and coma even with axial light. In addition to asymmetrical aberrations due to heat absorptions and aberrations due to characteristic changes on the beam splitting surface, accurate productions of the beam splitter is difficult.
The optical system disclosed in the references 8 to 10 propose a twice-imaging catadioptric optical system for forming an intermediate image once. It includes a first imaging optical system that has a reciprocating optical system (double-pass optical system) which includes concave mirrors to form an intermediate image of a first object (e.g., a reticle), and a second imaging optical system that forms the intermediate image onto a surface of a second object (e.g., a wafer). The optical system of the reference 8 arranges a first plane mirror near the intermediate image for deflecting an optical axis and light near the intermediate image. The deflected optical axis is made approximately parallel to a reticle stage and is deflected once again by a second plane mirror, or an image is formed onto a second object without a second plane mirror. In the optical system of the reference 9, a positive lens refracts light from a first object (e.g., a reticle), and a first plane mirror deflects the optical axis. A second plane mirror in a first imaging optical system again deflects the light reflected by a reciprocating optical system that includes a concave mirror to form an intermediate image. The intermediate image is projected onto a second object (e.g., a wafer) with a second imaging optical system. However, a magnification of the first imaging optical system serves as a reduction system more (corresponding to a paraxial magnification |β1| of about 0.625 of the first imaging optical system). Therefore, the first intermediate image enlarges the NA of the first intermediate image for an object-side NA in the first object by the reduction magnification. As a result, an incident angle range upon the plane mirror increases, and a higher NA scheme as in the immersion etc. encounters a serious problem. In other words, the first imaging optical system that controls a reduction magnification, a higher NA excessively increases the incident angle range upon the plane mirror, and a reflection film on the plane mirror causes a large difference in reflected light's intensity between the p-polarized light and s-polarized light. As a result, a critical dimension (“CD”) difference undesirably increases in an effective image plane. In the optical system of the reference 10, a first plane mirror deflects light from a first object (e.g., a reticle), a second plane mirror deflects the light reflected by a reciprocating optical system that includes a concave mirror, and a positive lens forms an intermediate image. The intermediate image is projected onto a second object (e.g., a wafer) with a second imaging optical system. Thus, a distance from the second plane mirror to the intermediate image becomes long by forming the intermediate image via the positive lens, and a light diameter on the second plane mirror becomes large. Therefore, an influence to a quality of the image projected onto the image surface by a few flaws exited on the reflection surface can be disregarded. Moreover, an asymmetry contribution to an imaging error such as coma generated by heating to the lens is compensated by arranging the positive lens in before and after the middle image and symmetry. However, it is difficult to control reflection film properties because the incident angle upon the plane mirror is large. In other words, the light intensity difference between the p-polarized light and s-polarized light increases by the influence of the reflection film on the plane mirror, and the CD difference in the effective image plane will be increased.
On the other hand, the optical system shown in
Accordingly, the present invention is directed to a catadioptric optical system, an exposure apparatus having the same, and device fabrication method, that can simplify a mechanical structure, minimize an influence of a reflection film on a plane mirror, reduce a physical interference between light and a lens according a higher NA and a chromatic coma aberration generated by a lens between a plane mirror and an intermediate image, and achieve a superior image performance.
A catadioptric optical system according to one aspect of the present invention includes a first imaging optical system including a concave mirror and forming an intermediate image of a first object, said first imaging optical system forming a reciprocating optical system that an incidence light and reflected light pass, a second imaging optical system for forming an image of the intermediate image onto a second object, and a first optical path deflective member, provided between the concave mirror and the intermediate image, for introducing a light from the first imaging optical system to the second imaging optical system, wherein said first optical path deflective member deflects a light in such a direction that a forward path of the first imaging optical system intersects a return path of the first imaging optical system, wherein said intermediate image is formed without an optical element after a deflection, and wherein the image of the first object is projected onto the second object through an intermediate image formation.
Other objects and further features of the present invention will become readily apparent from the following description of the preferred embodiments with reference to the accompanying drawings.
A description will now be given of a catadioptric projection optical system of one aspect according to the present invention, with reference to the accompanying drawings. In each figure, the same reference numeral denotes the same element. Therefore, a duplicate description will be omitted. Here,
Referring to
The catadioptical projection optical system 100 include, in order of light traveling from the first object 101 side, a first imaging optical system Gr1 and a second imaging optical system Gr2.
The first imaging optical system Gr1 includes a lens unit L1A, a concave mirror M1 arranged near a pupil position, and a reciprocating optical system (part) L1B, and forms a real image of the first object 101 (a first intermediate image IMG1). A first deflective reflector FM1 is inclined to the optical axis AX1 at 45°, deflects light from the first imaging optical system Gr1 and introduces to the second imaging optical system Gr2. A second deflective reflector FM2 is inclined to the optical axis AX2 at 45 and deflects light from the intermediate image IMG. Thereby, it is possible to arrange the first object 101 and the second object 102 in parallel. In
The second imaging optical system Gr2 includes a lens unit L2A and a lens unit L2B. The second imaging optical system Gr2 has a pupil in the lens unit L2B and forms an image of the intermediate image IMG onto the second object 102 at a predetermined magnification.
The first imaging optical system's concave mirror M1 and lens correct chromatic aberrations and a positive Petzval sum generated by the second imaging optical system Gr2.
In the catadioptric projection optical system 100 of the present invention, the first deflective reflector FM1 deflects, as shown in
The catadioptric projection optical system 100 reflects light by the first deflective reflector FM1 and forms an intermediate image IMG without through the lens. Therefore, the catadioptric projection optical system 100 can avoid interference between a marginal ray of the first imaging optical system Gr1 and the lens unit L2A, and a structure of an optical system becomes easy for a higher NA.
The catadioptric projection optical system 100 does not arrange the lens between the first deflective reflector FM1 and the second deflective reflector FM2, but arranges the lens between the intermediate image IMG and the second deflective reflector FM2. Therefore, the catadioptric projection optical system 100 can obtain effects that compensate a coma generated in the lens near the second object 102 that becomes a problem to a higher NA.
In the catadioptric projection optical system 100, preferably, the following conditional expression, where β1 is a paraxial imaging magnification of the first imaging optical system Gr1, and NAO is a numerical aperture of the light at the first object 101 side.
|β1/NAO|>3.8 (1)
The conditional expression (1) defines a ratio between the paraxial imaging magnification of the first imaging optical system Gr1 and the numerical aperture NAO at the first object 101 side. If a value is lower than the lower limit in the conditional expression (1), the imaging magnification β1 of the first imaging optical system Gr1 becomes an excessively small reduction magnification and a principal ray angle and an incident angle range of the light entering the first deflective reflector FM1 become excessively large. The excessively large incident angle range undesirably complicates control over reflection film properties of a plane mirror. A transmittance distribution on a pupil changes and the imaging performance deteriorates.
In the ratio between the paraxial imaging magnification of the first imaging optical system Gr1 and the numerical aperture of the light NAO at the first object 101 side, more preferably, the following conditional expression is met.
6.2>|β1/NAO|>5.0 (2)
If a value is exceeds the upper limit in the conditional expression (2), the imaging magnification β1 of the first imaging optical system Gr1 becomes an excessively large reduction magnification, a light diameter on the first deflective reflector FM1 becomes excessively large, and light on the forward path is limited. Therefore, it is difficult to secure an enough effective imaging area.
On the other hand, if a value is satisfied the lower limit of the conditional expression (2), the principal ray angle and the incident angle range of the light entering the first deflective reflector FM1 can controlled to small. Therefore, it is easy to control reflection film properties of the plane mirror.
In the catadioptric projection optical system 100, preferably, the following conditional expression, where β1 is a paraxial imaging magnification of the first imaging optical system Gr1, βf is a paraxial imaging magnification of the lens unit L2A arranged between the intermediate image IMG and the second deflective reflector FM2, and NAO is a numerical aperture of the light at the first object 101 side.
6.80<|β1·βf/NAO|<10.60 (3)
If a value is lower than the lower limit in the conditional expression (3), a imaging magnification from the first imaging optical system Gr1 to the lens unit L2A becomes an excessively small reduction magnification and a principal ray angle and an incident angle range of the light entering the second deflective reflector FM2 become excessively large. The excessively large incident angle range undesirably complicates control over reflection film properties of a plane mirror. A transmittance distribution on a pupil changes and the imaging performance deteriorates.
If a value exceeds the upper limit in the conditional expression (3), the imaging magnification from the first imaging optical system Gr1 to the lens unit L2A becomes an excessively large reduction magnification, and it is necessary to become the imaging magnification of second imaging optical system Gr2 to excessively small. Therefore, it is necessary to become the power to large because the pupil moves the first object 101 side, and the Petzval sum deteriorates.
Moreover, in the catadioptric projection optical system 100, preferably, the following conditional expression, where a is a distance parallel to the optical axis AX2 between the intermediate image IMG and a first surface of an optical element closest to the intermediate image IMG among the lens unit L2A, and b is a distance along the optical axis AX2 and the optical axis AX3 for the light from the intermediate image IMG to the second object 102 surface via the second imaging optical system Gr2.
0.0005<a/b<0.105 (4)
If a value is lower than the lower limit of the conditional expression (4), the first imaging optical system Gr1 and the lens unit L2A close, it is difficult to secure a space, and results in complicating a mechanical structure. The correcting effect of the chromatic coma aberration decreases.
On the other hand, if a value exceeds the upper limit of the conditional expression (4), an effective diameter of lens of the lens unit L2A becomes excessively large. The excessively large effective diameter of lens undesirably complicates manufacture of high quality lens materials, and the apparatus becomes big.
In addition, in the catadioptric projection optical system 100, preferably, the following conditional expression, where c is a distance along the optical axis AX1, the optical axis AX2 and the optical axis AX3 for the light from the first surface 101 to the second object 102 surface via the optical elements.
0.47<b/c<0.58 (5)
If a value is lower than the lower limit of the conditional expression (5), a space between the first imaging optical system Gr1 and the second imaging optical system Gr2 becomes narrow, and results in complicating a mechanical structure. On the other hand, if a value exceeds the upper limit of the conditional expression (5), an effective diameter of lens of the second imaging optical system Gr2 becomes excessively large. The excessively large effective diameter of lens undesirably complicates manufacture of high quality lens materials, and the apparatus becomes big.
A sign of an angle of a pupil paraxial ray may be inverted at before or after the lens unit L2A arranged between the intermediate image IMG and the second deflective reflector FM2. If the sign is not inverted, the incident angle of the principal ray entering the second deflective reflector FM2 becomes excessively large. The excessively large incident angle undesirably complicates control over reflection film properties of the plane mirror.
An angle between a principal ray of light incident upon the first deflective reflector FM1 and a reflection surface of the first deflective reflector FM1 may be 43° or smaller. Because a convergent light incident upon the first deflective reflector FM1, the marginal ray is incident upon the first deflective reflector FM1 by a larger angle than the principal ray. The incident angle may be small from viewpoint of the reflection film on the plane mirror. Therefore, the incident angle of off-axis principal ray becomes 43° or smaller to the first deflective reflector FM1 inclined to the optical axis AX1 at 45°.
The incident angle range may be small to control reflection film properties formed on the plane mirror. Therefore, the incident angle range of ray entering the first deflective reflector FM1 is preferably 35° or smaller, more preferably 30° or smaller.
In the catadioptric projection optical system 100, all positive power optical elements arranged between the first deflective reflector FM1 and the second deflective reflector FM2 have an expansion magnification. In other words, the positive power optical element only arranges between the intermediate image IMG as the real image and the second deflective reflector FM2. Thereby, the correcting effect of the chromatic coma aberration can be obtained, and the incident angle and the incident angle range of light entering the second deflective reflector FM2 decrease. Therefore, it is easy to control reflection film properties of the plane mirror.
In the catadioptric projection optical system 100, preferably, the following conditional expression is met, where β1 is the paraxial imaging magnification of the first imaging optical system Gr1.
|β1>1.0 (6)
If a value is lower than the lower limit of the conditional expression (6), the imaging magnification β1 of the first imaging optical system Gr1 becomes an excessively small reduction magnification and the incident angle range of the light entering the first deflective reflector FM1 become excessively large. The excessively large incident angle range undesirably complicates control over reflection film properties of a plane mirror.
In the paraxial imaging magnification β1 of the first imaging optical system Gr1, more preferably, the following conditional expression is met.
1.25>β1 (7)
If the conditional expression (7) is not met, a light diameter on the first deflective reflector FM1 becomes excessively large, and light on the forward path is limited. Therefore, it is difficult to secure an enough effective imaging area.
In
An angle between the optical axis AX1 and the reflection surface of the first deflective reflector FM1 is preferably 45° or smaller. If the angle is not 45° or smaller, the incident angle of ray entering the first deflective reflector FM1 becomes large, and it is difficult to control reflection film properties of the plane mirror. Moreover, it is difficult to secure a space near the first object 101, and results in complicating a mechanical structure.
A shortest distance parallel to the optical axis AX2 between an optical element of the first imaging optical system Gr1 or marginal ray and a first surface of a lens closest to the first imaging optical system Gr1 among the lens unit L2A is preferably 30 mm or more. If the shortest distance is not 30 mm or more, a physical interference with light and lens occurs, and results in complicating a mechanical structure.
The upper limit of the shortest distance parallel to the optical axis AX2 between the optical element of the first imaging optical system Gr1 or marginal ray and the first surface of the lens closest the first imaging optical system Gr1 among the lens unit L2A is more preferably 160 mm or less. If the shortest distance exceeds 160 mm, the intermediate image IMG and the lens unit L2A excessively separates from each other, and the effective diameter of the lens unit L2A becomes excessively large. The excessively large effective diameter of lens undesirably complicates manufacture of high quality lens materials, and the apparatus becomes big.
If the intermediate image IMG and the lens unit L2A closes from each other, it is necessary to separate the first deflective reflector FM1 and the intermediate image IMG from each other. Therefore, the light diameter on the first deflective reflector FM1 becomes excessively large, and light on the forward path is limited. Thereby, it is difficult to secure an enough effective imaging area. A higher object point of the first object 101 to secure the effective imaging area is not desirable because correcting the aberration becomes difficult.
The catadioptric projection optical system 100 includes, in the present embodiment, deflective reflectors (the first deflective reflector FM1 and the second deflective reflector FM2). Concretely, the catadioptric projection optical system 100 has one deflective reflector respectively in the optical path of the first imaging optical system Gr1 and the optical path of the second imaging optical system Gr2. Here, when the first object 101 and the second object 102 are arranged in abbreviation parallel, the first deflective reflector FM1 and the second deflective reflector FM2 are arranged to form a relative angle difference of 90° between their reflective surfaces. When the first object 101 and the second object 102 do not need to be arranged in abbreviation parallel, the second deflective reflector FM2 does not need to arrange.
For the catadioptric projection optical system 100 of the present invention, the first imaging optical system Gr1 includes the reciprocating optical system (part) L1B. However, the reciprocating optical system L1B has a negative refractive power and includes at least one lens having a negative refractive power. At least one of those lenses having a negative refractive power preferably have its concave surface oriented toward the first object 101. This reciprocating optical system L1B preferably has at least one lens having an aspheric surface. If the reciprocating optical system L1B does not have the lens having the aspheric surface, a plurality of lenses are used for the reciprocating optical system L1B to share the power. Of course, even when the lens having the aspheric surface is used, constructing the reciprocating optical system L1B with a plurality of lenses can better control introduction of aberrations at the reciprocating optical system part. The concave mirror M1 may have an aspheric surface.
The first deflective reflector FM1 and the second deflective reflector FM2 include deflective mirrors. The shape of the deflective mirror may be a shape of a flat plate or other shape (for example, part of a cubic shape). The first deflective reflector FM1 and the second deflective reflector FM2 may also be a mirror that utilizes backside reflection of glass. The light splitter may also be used for the first deflective reflector FM1 and the second deflective reflector FM2, in which case, an off-axial beam can be used from the on-axis.
An aperture stop (not shown) is preferably arranged in the second imaging optical system Gr2. The aperture stop may also be arranged in combination or singly around where a principal ray of the first imaging optical system Gr1 intersects the optical axis AX1.
In
In the catadioptric projection optical system 100, preferably, at least the image-surface side is made telecentric to reduce fluctuations of the magnification when a surface of the second object 102 varies in the optical-axis direction.
Preferably, the catadioptric projection optical system 100 provides the first imaging optical system Gr1 with the concave mirror M1 and a refractor, the second imaging optical system Gr2 with a refractor. The catadioptric system when used for the final imaging optical system causes interfere between a concave mirror and the light, and complicates a configuration of an optical system with a high NA. If a catadioptric system is not adopted as a subsystem in the total optical system, chromatic aberrations are hard to be corrected. Moreover, if a reflective system is used for the first imaging optical system Gr1, chromatic aberrations are hard to be corrected.
The catadioptric projection optical system 100 may include an aberration correction mechanism that corrects aberrations. The aberration correction mechanism is possible to include a mechanism in the first imaging optical system Gr1 that moves a lens in an optical axis direction and/or in a direction vertical to an optical axis, or in other directions (to decenter a lens). A similar aberration correction mechanism may be included in the second imaging optical system Gr2. In addition, a mechanism for deforming the concave mirror M1 may be included to correct aberrations.
The catadioptric projection optical system 100 is suitable an immersion structure that fills a fluid between the second object 102 surface and the final lens surface of the optical system. However, the space between the second object 102 surface and the final lens surface may be air.
A field stop may be provided near the intermediate image IMG. When a diffraction optical element is used for the optical system, and the second object 102 surface and its neighborhood use the above immersion structure, a view-field limiting stop provided to a final glass surface on the optical system and a neighboring field stop (e.g., between the final glass surface and the surface of the second object 102) will prevent flare light etc., which are and are not generated from the diffraction optical element, from arriving at the second object 102 surface. The second object 102 surface may have an immersion structure without employing a diffraction optical element in the optical system.
In building an immersion optical system, whether or not a diffraction optical element is present, an axial interval between the final surface of the optical system and the surface of the second object 102 is preferably 5 mm or less, more preferably 2 mm or less, to minimize influences by fluid properties etc. on the imaging performance of the optical system.
Although the catadioptric projection optical system 100 has, in the instant embodiment, a magnification of ¼, it is not limited to this and may be 1/5 or 1/6.
The catadioptric projection optical system 100 uses an off-axial image point of the first object, in a certain range off the optical axis. At that time, a rectangular or arc slit area on the first object surface, not inclusive of the optical axis, becomes an exposure area.
The catadioptric projection optical system 100 deflects light on the return path of the reciprocating optical system in a direction that intersects light on the forward path by the first deflective reflector FM1. Therefore, the deterioration of the reflection film properties resulting from the incident angle range upon the deflective reflector that becomes the problem according a shorter wavelength and a higher NA can be prevented. The catadioptric projection optical system 100 reflects light by the first deflective reflector FM1 and forms the intermediate image IMG without through the lens. Therefore, the incident angle range upon the second deflective reflector FM2 decreases, and it is easy to control the reflection film properties. Moreover, the catadioptric projection optical system 100 avoids interference between light near the intermediate image and the lens, control the chromatic coma aberration, and can be obtain the predetermined imaging performance. However, the catadioptric projection optical system 100 is not limited to the structure shown in
The catadioptric projection optical system 100 of the present invention is especially effective with a high NA of 0.8 or higher, particularly, 0.85 or higher. The catadioptric projection optical system 100 of the present invention is suitable for the exposure apparatus that uses a light with shorten wavelength, preferably a light with a wavelength of 200 nm or less, as exposure light, and is especially effective for the wavelength such as ArF excimer laser and F2 laser that requires for to the immersion.
Hereafter, a description will be given of a configuration of the catadioptric projection optical system 100.
The first imaging optical system Gr1 includes, in order from the first object 101 side, a lens unit L1A having a positive refractive power, a reciprocating optical system (part) L1B having a negative refractive power, and a concave mirror M1.
The lens unit L1A includes, along the light traveling direction from the side of the first object 101, an aspheric positive lens L111 and a positive lens L112. The aspheric positive lens L111 has an approximately planoconvex form that has a convex surface oriented toward the first object 101 side. The positive lens L112 has a meniscus form that has a convex surface oriented toward a side opposite to the first object 101 side.
The reciprocating optical system L1B includes an aspheric negative lens L113, a positive lens L114, an aspheric negative lens L115, a negative lens L116, and a concave mirror M1. The aspheric negative lens L113 has an approximately planoconcave form that has a concave surface oriented toward a side opposite to the first object 101 side. The positive lens L114 has an approximately planoconvex form that has a convex surface oriented toward the first object 101 side. The aspheric negative lens L115 has a meniscus form that has a concave mirror oriented toward the first object 101 side. The negative lens L116 has a meniscus form that has a concave surface oriented toward the first object 101 side. The concave mirror M1 has a concave form that has a concave surface oriented toward the first object 101 side.
The light from the first object 101 passes through the lens unit L1A, enters the reciprocating optical system L1B, is reflected at the concave mirror M1, and reenters the reciprocating optical system L1B. Then, a deflective reflector FM1 deflects the optical axis AX1 to the optical axis AX2 by 90°. The light is also reflected, and an intermediate image IMG is formed.
The first deflective reflector FM1 is arranged between the first imaging optical system Gr1 and the second imaging optical system Gr2. Preferably, as in the instant embodiment, the first deflective reflector FM1 is arranged between the intermediate image IMG and the reciprocating optical system L1B. In the instant embodiment, the first deflective reflector FM1 uses a flat mirror.
The second imaging optical system Gr2 includes a lens unit L2A having a positive refractive power and a lens unit L2B having a positive refractive power.
The lens unit L2A includes, along the light traveling direction from the side of the first imaging optical system Gr1, a biconvex aspheric positive lens L211 and a meniscus aspheric positive lens L212 with its convex surface oriented toward a side opposite to the intermediate image IMG side.
The lens unit L2B includes a positive lens L213, a negative lens L214, an aspheric positive lens L215, an aspheric positive lens L216, a negative lens L217, an aspheric positive lens L218, an aspheric positive lens L219, an aperture stop 103, a positive lens L220, a positive lens L221, an aspheric positive lens L222, a positive lens L223, an aspheric positive lens L224, and an aspheric positive lens L225. The positive lens L213 has a meniscus form that has a convex surface oriented toward the second object 102 side. The negative lens L214 has a biconcave form. The aspheric positive lens L215 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L216 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The negative lens L217 has an approximately planoconcave form that has a concave surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L218 has a meniscus form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L219 has a biconvex form. The positive lens L220 has a meniscus form that has a convex surface oriented toward the second object 102 side. The positive lens L221 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L222 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The positive lens L223 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L224 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L225 has a planoconvex form that has a plane surface oriented toward the second object 102 side.
The second deflective reflector FM2 is arranged between the lens unit L2A and the lens unit L2B of the second imaging optical system Gr2. The present embodiment makes the second deflective reflector FM2 of a plane mirror for deflecting the light reflected from the first deflective reflector FM1 in a predetermined direction.
The second imaging optical system Gr2 of the instant embodiment includes, but is not limited to, the lens unit L2A having positive refractive power and the lens unit L2B having positive refractive power. For example, the lens unit L2B can have a lens unit with a negative refractive power or another structure.
The aperture stop 103 is arranged between the aspheric positive lens L219 and the positive lens L220.
The catadioptric projection optical system 100 of the first embodiment uses a projection magnification of ¼, a reference wavelength of 157 nm, and calcium fluoride as a glass material. An image-side numerical aperture is NA=0.80. An object-image distance (the first object 101 surface to the second object 102 surface) is L=997.84 mm. An aberration-corrected object point in a range of about 7.50 to 20.25 mm secures a rectangular exposure area of at least 26 mm long and 8 mm wide.
The following Table 1 shows the specification of the numerical example of the catadioptric projection optical system 100 of the first embodiment. “i” in the table is a surface number along a direction of light traveling from the first object 101. “ri” is a radius of curvature for each surface corresponding to a surface number. “di” is a surface spacing of each surface. A shape of an aspheric surface is given by the following equation:
X=(H2/4)/(1+((1−(1+k)·(H/ri)2))½)+AH4+BH6+CH8+DH10+EH12+FH14+GH16
where X is a displacement in a direction of an optical axis from the lens top, H is a distance from the optical axis, ri is a radius of curvature, k is a conical constant; and A, B, C, D, E, F, and G are aspheric coefficients. A lens glass material CaF2 has a refractive index to a reference wavelength λ=157.000 nm is 1.56. The refractive indexes of the wavelengths of +0.6 pm and −0.6 pm for the reference wavelengths are, 1.55999847 and 1.560000153, respectively.
TABLE 1
DISTANCE FROM FIRST OBJECT~FIRST
SURFACE: 41.15312 mm
LENS
i
ri
di
MATERIAL
1
395.97465
20.22118
caf2
2
−2898.20269
44.71464
3
−251.61654
42.00000
caf2
4
−231.04782
286.07966
5
−1822.70249
28.34838
caf2
6
256.11745
10.06127
7
254.50945
35.66908
caf2
8
−2557.13314
103.60600
9
−180.38280
20.31823
caf2
10
−468.06841
10.69468
11
−339.05921
21.00642
caf2
12
−1135.87333
33.83254
13
−278.56064
−33.83254
M1
14
−1135.87333
−21.00642
caf2
15
−339.05921
−10.69468
16
−468.06841
−20.31823
caf2
17
−180.38280
−103.60600
18
−2557.13314
−35.66908
caf2
19
254.50945
−10.06127
20
256.11745
−28.34838
caf2
21
−1822.70249
−268.88082
22
0.00000
162.32865
FM1
23
412.14379
44.81415
caf2
24
−514.47810
24.63586
25
−350.11325
33.47520
caf2
26
−254.60012
219.66548
27
0.00000
−199.95918
FM2
28
514.92997
−23.66212
caf2
29
255.35596
−13.37135
30
338.01319
−15.04140
caf2
31
−459.91711
−1.01570
32
−258.57016
−34.83108
caf2
33
−457.51166
−71.87340
34
−223.68365
−47.54530
caf2
35
751.85440
−22.60074
36
268.47191
−23.38703
caf2
37
−1165.25792
−16.20487
38
−386.40525
−20.33655
caf2
39
−466.36508
−12.77442
40
−370.27173
−63.27240
caf2
41
232.77226
23.91356
42
0.00000
−42.90082
APERTURE STOP
43
1148.49808
−68.29475
caf2
44
568.06929
−1.01683
45
−219.12809
−49.17786
caf2
46
1682.72634
−1.01683
47
−514.87058
−21.29114
caf2
48
−39003.71488
−2.51668
49
−616.56989
−17.52530
caf2
50
−3.5E+05
−1.83409
51
−910.87500
−24.55409
caf2
52
−11464.91757
−1.01683
53
−209.21733
−49.49135
caf2
54
0.00000
−9.95147
L = 997.84 mm
β = ¼
NA = 0.80
|β1/NAO| = 5.29
|β1 · βf/NAO| = 7.65
|β1| = 1.057
a/b = 0.0538
b/c = 0.479
ASPHERICAL SURFACES
i
K
A
B
C
1
0.67157400
−3.12148340E−09
1.24961887E−13
−1.07206311E−17
6
−0.26422545
−4.07630359E−09
−3.74292072E−13
−1.46846516E−17
10
−0.04052878
−5.40216034E−09
1.46578961E−13
6.53664151E−20
16
−0.04052878
−5.40216034E−09
1.46578961E−13
6.53664151E−20
20
−0.26422545
−4.07630359E−09
−3.74292072E−13
−1.46846516E−17
23
−0.06868808
−1.05721576E−08
−4.79962790E−14
4.74439039E−19
25
1.04273198
−4.70121479E−09
1.07389747E−13
1.24811271E−18
32
−1.01492628
−1.96968709E−08
2.44323828E−13
−4.76571749E−18
34
−0.45182630
2.12897818E−08
2.93116566E−13
1.54392512E−17
39
−1.99465650
−3.89130899E−08
5.64229062E−13
7.10821780E−18
41
−1.09917187
−1.56104003E−08
6.72159485E−13
−3.21066701E−17
47
1.46551924
5.88942104E−08
3.79528671E−12
−2.62771281E−16
51
−2.04763264
−6.93796147E−08
−3.23034550E−12
8.79032313E−16
53
−0.58689189
−4.47928864E−08
1.18331479E−13
−2.99578474E−16
i
D
E
F
G
1
3.02396381E−21
−4.17118053E−25
2.78125431E−29
−6.44187470E−34
6
2.12902413E−21
−2.81497785E−25
1.50694792E−29
−3.53816272E−34
10
2.55935824E−22
−2.01752638E−27
−4.05301590E−31
2.49240398E−35
16
2.55935824E−22
−2.01752638E−27
−4.05301590E−31
2.49240398E−35
20
2.12902413E−21
−2.81497785E−25
1.50694792E−29
−3.53816272E−34
23
−8.39315466E−22
4.89327799E−26
−1.86906734E−30
−1.91328722E−36
25
3.43732001E−22
−7.17783414E−28
−2.94948641E−31
3.96862254E−35
32
−5.04835667E−22
6.49443358E−26
−3.00384245E−30
6.50850163E−35
34
4.13121834E−22
−3.42060737E−26
3.13448029E−30
−1.26160384E−34
39
3.92603930E−22
−8.05151085E−26
2.70060158E−30
−5.33417169E−35
41
1.37582551E−21
−5.72809395E−26
1.81888057E−30
−1.90531697E−35
47
−1.60589201E−20
2.16600278E−24
−9.01334418E−29
1.30281885E−33
51
−4.52726701E−20
5.98777721E−24
−4.25816067E−28
1.53629738E−32
53
−2.91098686E−19
7.52634824E−23
−1.41750767E−26
8.34861881E−31
The first imaging optical system Gr1 includes, in order from the first object 101 side, a lens unit L1A having a positive refractive power, a reciprocating optical system (part) L1B having a negative refractive power, and a concave mirror M1.
The lens unit L1A includes, along the light traveling direction from the side of the first object 101, an aspheric positive lens L111 and a positive lens L112. The aspheric positive lens L111 has a biconvex form. The positive lens L112 has a meniscus form that has a convex surface oriented toward a side opposite to the first object 101 side.
The reciprocating optical system L1B includes an aspheric negative lens L113, a positive lens L114, an aspheric negative lens L115, a negative lens L116, and a concave mirror M1. The aspheric negative lens L113 has an approximately planoconcave form that has a concave surface oriented toward a side opposite to the first object 101 side. The positive lens L114 has an approximately planoconvex form that has a convex surface oriented toward the first object 101 side. The aspheric negative lens L115 has a meniscus form that has a concave mirror oriented toward the first object 101 side. The negative lens L116 has a meniscus form that has a concave surface oriented toward the first object 101 side. The concave mirror M1 has a concave form that has a concave surface oriented toward the first object 101 side.
The light from the first object 101 passes through the lens unit L1A, enters the reciprocating optical system L1B, is reflected at the concave mirror M1, and reenters the reciprocating optical system L1B. Then, a deflective reflector FM1 deflects the optical axis AX1 to the optical axis AX2 by 90°. The light is also reflected, and an intermediate image IMG is formed.
The first deflective reflector FM1 is arranged between the first imaging optical system Gr1 and the second imaging optical system Gr2. Preferably, as in the instant embodiment, the first deflective reflector FM1 is arranged between the intermediate image IMG and the reciprocating optical system L1B. In the instant embodiment, the first deflective reflector FM1 uses a flat mirror.
The second imaging optical system Gr2 includes a lens unit L2A having a positive refractive power and a lens unit L2B having a positive refractive power.
The lens unit L2A includes, along the light traveling direction from the side of the first imaging optical system Gr1, a biconvex aspheric positive lens L211 and a meniscus aspheric positive lens L212 with its convex surface oriented toward a side opposite to the intermediate image IMG side.
The lens unit L2B includes a positive lens L213, a negative lens L214, an aspheric positive lens L215, an aspheric positive lens L216, a negative lens L217, an aspheric positive lens L218, an aspheric positive lens L219, an aperture stop 103, a positive lens L220, a positive lens L221, an aspheric negative lens L222, a positive lens L223, an aspheric positive lens L224, and an aspheric positive lens L225. The positive lens L213 has a meniscus form that has a convex surface oriented toward the second object 102 side. The negative lens L214 has a biconcave form. The aspheric positive lens L215 has a meniscus form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L216 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The negative lens L217 has a biconcave form. The aspheric positive lens L218 has a meniscus form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L219 has a biconvex form. The positive lens L220 has a meniscus form that has a convex surface oriented toward the second object 102 side. The positive lens L221 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric negative lens L222 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The positive lens L223 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L224 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L225 has a planoconvex form that has a plane surface oriented toward the second object 102 side.
The second deflective reflector FM2 is arranged between the lens unit L2A and the lens unit L2B of the second imaging optical system Gr2. The present embodiment makes the second deflective reflector FM2 of a plane mirror for deflecting the light reflected from the first deflective reflector FM1 in a predetermined direction.
The aperture stop 103 is arranged between the aspheric positive lens L219 and the positive lens L220.
The catadioptric projection optical system 100 of the second embodiment uses a projection magnification of ¼, a reference wavelength of 157 nm, and calcium fluoride as a glass material. An image-side numerical aperture is NA=0.80. An object-image distance (the first object 101 surface to the second object 102 surface) is L=1051.59 mm. An aberration-corrected object point in a range of about 7.50 to 20.25 mm secures a rectangular exposure area of at least 26 mm long and 8 mm wide.
The following Table 2 shows the specification of the numerical example of the catadioptric projection optical system 100 of the second embodiment. Symbols in the table are the same as in table 1, and thus a description thereof will be omitted.
TABLE 2
DISTANCE FROM FIRST OBJECT~FIRST
SURFACE: 69.87426 mm
LENS
i
ri
di
MATERIAL
1
668.40243
20.22118
caf2
2
−909.99969
20.15953
3
−278.78157
41.82957
caf2
4
−226.53067
306.96914
5
−9013.50255
21.17315
caf2
6
227.11071
14.30268
7
252.59236
32.41133
caf2
8
3060.02052
91.62181
9
−251.66991
20.06219
caf2
10
−657.64908
16.70481
11
−298.52631
20.01564
caf2
12
−1155.92042
27.46979
13
−277.46695
−27.46979
M1
14
−1155.92042
−20.01564
caf2
15
−298.52631
−16.70481
16
−657.64908
−20.06219
caf2
17
−251.66991
−91.62181
18
3060.02052
−32.41133
caf2
19
252.59236
−14.30268
20
22.11071
−21.17315
caf2
21
−9013.50255
−292.82106
22
0.00000
144.98564
FM1
23
504.78955
42.62735
caf2
24
−475.98929
158.10011
25
−803.47768
40.00000
caf2
26
−340.39441
99.24315
27
0.00000
−200.01742
FM2
28
627.21306
−24.57765
caf2
29
275.15619
−2.32909
30
434.05214
−17.83341
caf2
31
−685.95720
−1.00000
32
−266.06165
−40.00000
caf2
33
−236.39777
−98.47464
34
−201.23101
−52.61738
caf2
35
998.68752
−20.80028
36
428.05968
−23.38703
caf2
37
−330.13594
−34.04513
38
−398.32107
−20.33655
caf2
39
−1741.28350
−24.68386
40
−465.91801
−68.95155
caf2
41
214.11384
28.60841
42
0.00000
−46.19472
APERTURE STOP
43
2389.68736
−67.41845
caf2
44
666.87372
−1.01683
45
−213.66192
−44.46924
caf2
46
954.85885
−1.01683
47
−795.17615
−20.28664
caf2
48
−550.11819
−3.06249
49
−349.24693
−17.50613
caf2
50
−16687.89701
−2.30561
51
−925.70468
−24.79031
caf2
52
−47751.77910
−1.01683
53
−190.68875
−45.82729
caf2
54
0.00000
−9.99596
L = 1051.59 mm
β = ¼
NA = 0.80
|β1/NAO| = 6.11
|β1 · βf/NAO| = 8.15
|β1| = 1.222
a/b = 0.00088
b/c = 0.470
ASPHERICAL SURFACES
i
K
A
B
C
1
1.84472719
−4.28737069E−09
−4.41427710E−14
8.11274173E−18
6
−0.27189589
−4.22360534E−09
−3.66149757E−13
−5.21688557E−18
10
0.49938484
−6.02516745E−09
1.48782891E−13
−9.03391986e−019
16
0.49938484
−6.02516745E−09
1.48782891E−13
9.03391986E−19
20
−0.27189589
−4.22360534E−09
−3.66149757E−13
−5.21688557E−18
23
0.79344720
−9.58055891E−09
−1.44694100E−13
1.99136296E−17
25
0.38159869
−7.27012352E−09
7.67976427E−14
−2.01234702E−19
32
−0.46697051
−2.04044049E−08
3.74018192E−13
−1.16647192E−17
34
−0.53480624
2.26188296E−08
2.79329047E−13
1.85357176E−17
39
−1.08351559
−3.95543216E−08
2.30977379E−13
9.83209623E−18
41
−0.95966217
−1.45575701E−08
7.81477775E−13
−3.03683767E−17
47
−0.95442908
5.47250405E−08
4.34318997E−12
−2.78298594E−16
51
−1.96075510
−9.49376715E−08
−3.00111451E−12
5.98641043E−16
53
−1.17537128
−1.33444944E−08
4.64806503E−12
−2.23525496E−16
i
D
E
F
G
1
−2.07377580E−21
2.14738504E−25
−1.19376730E−29
3.39039856E−34
6
1.44705561E−21
−1.96777906E−25
1.14310793E−29
−2.72077599E−34
10
−3.13004905E−24
2.20935958E−26
−1.66002358E−30
5.39928337E−35
16
−3.13004905E−24
2.20935958E−26
−1.66002358E−30
5.39928337E−35
20
1.44705561E−21
−1.96777906E−25
1.14310793E−29
−2.72077599E−34
23
−1.84064584E−21
1.07963092E−25
−3.78934188E−30
5.69453371E−35
25
9.84789574E−23
−7.73186611E−27
2.70919906E−31
−5.25476041E−36
32
3.68781098E−22
7.76457500E−28
−3.63007208E−31
1.53597787E−35
34
2.89666734E−22
−2.25156851E−26
2.54901422E−30
−1.14638254E−34
39
1.67679893E−22
−2.86823967E−26
−6.87337289E−31
9.61735989E−36
41
1.39961175E−21
−5.53226831E−26
1.81465248E−30
−2.39708052E−35
47
−1.07107681E−20
1.28989008E−24
−2.57193395E−29
−6.39379334E−34
51
−2.74686808E−20
7.84557981E−24
−8.32541969E−28
6.57146205E−32
53
−2.70340899E−19
1.28545363E−23
−1.76779835E−27
−1.06366211E−30
The first imaging optical system Gr1 includes, in order from the first object 101 side, a lens unit L1A having a positive refractive power, a reciprocating optical system (part) L1B having a negative refractive power, and a concave mirror M1.
The lens unit L1A includes, along the light traveling direction from the side of the first object 101, an aspheric positive lens L111 and a positive lens L112. The aspheric positive lens L111 has an approximately planoconvex form that has a convex surface oriented toward the first object 101 side. The positive lens L112 has a meniscus form that has a convex surface oriented toward a side opposite to the first object 101 side.
The reciprocating optical system L1B includes an aspheric negative lens L113, a positive lens L114, an aspheric negative lens L115, a negative lens L116, and a concave mirror M1. The aspheric negative lens L113 has a biconcave form. The positive lens L114 has an approximately planoconvex form that has a convex surface oriented toward the first object 101 side. The aspheric negative lens L115 has a meniscus form that has a concave mirror oriented toward the first object 101 side. The negative lens L116 has a meniscus form that has a concave surface oriented toward the first object 101 side. The concave mirror M1 has a concave form that has a concave surface oriented toward the first object 101 side.
The light from the first object 101 passes through the lens unit L1A, enters the reciprocating optical system L1B, is reflected at the concave mirror M1, and reenters the reciprocating optical system L1B. Then, a deflective reflector FM1 deflects the optical axis AX1 to the optical axis AX2 by 90°. The light is also reflected, and an intermediate image IMG is formed.
The first deflective reflector FM1 is arranged between the first imaging optical system Gr1 and the second imaging optical system Gr2. Preferably, as in the instant embodiment, the first deflective reflector FM1 is arranged between the intermediate image IMG and the reciprocating optical system L1B. In the instant embodiment, the first deflective reflector FM1 uses a flat mirror.
The second imaging optical system Gr2 includes a lens unit L2A having a positive refractive power and a lens unit L2B having a positive refractive power.
The lens unit L2A includes, along the light traveling direction from the side of the first imaging optical system Gr1, an aspheric positive lens L211 and an aspheric positive lens L212. The aspheric positive lens L211 has a biconvex form. The aspheric positive lens L212 has a meniscus form that has a convex surface oriented toward a side opposite to the intermediate image IMG side.
The lens unit L2B includes a positive lens L213, a negative lens L214, an aspheric positive lens L215, an aspheric positive lens L216, a negative lens L217, an aspheric positive lens L218, an aperture stop 103, an aspheric positive lens L219, a positive lens L220, a positive lens L221, an aspheric positive lens L222, a positive lens L223, an aspheric positive lens L224, and an aspheric positive lens L225. The positive lens L213 has a meniscus form that has a convex surface oriented toward the second object 102 side. The negative lens L214 has a biconcave form. The aspheric positive lens L215 has a meniscus form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L216 has a biconvex form. The negative lens L217 has an approximately planoconcave form that has a concave surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L218 has a meniscus form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L219 has a biconvex form. The positive lens L220 has an approximately planoconvex form that has a convex surface oriented toward the second object 102 side. The positive lens L221 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L222 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The positive lens L223 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L224 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L225 has a planoconvex form that has a plane surface oriented toward the second object 102 side.
The second deflective reflector FM2 is arranged between the lens unit L2A and the lens unit L2B of the second imaging optical system Gr2. The present embodiment makes the second deflective reflector FM2 of a plane mirror for deflecting the light reflected from the first deflective reflector FM1 in a predetermined direction.
The aperture stop 103 is arranged between the aspheric positive lens L218 and the aspheric positive lens L219.
The catadioptric projection optical system 100 of the third embodiment uses a projection magnification of ¼, a reference wavelength of 157 nm, and calcium fluoride as a glass material. An image-side numerical aperture is NA=0.80. An object-image distance (the first object 101 surface to the second object 102 surface) is L=983.40 mm. An aberration-corrected object point in a range of about 7.50 to 20.25 mm secures a rectangular exposure area of at least 26 mm long and 8 mm wide.
The following Table 3 shows the specification of the numerical example of the catadioptric projection optical system 100 of the third embodiment. Symbols in the table are the same as in Table 1, and thus a description thereof will be omitted.
TABLE 3
DISTANCE FROM FIRST OBJECT~FIRST
SURFACE: 40.13403 mm
LENS
i
ri
di
MATERIAL
1
260.11007
20.22118
caf2
2
883.38340
28.09241
3
−591.69377
15.01918
caf2
4
−368.85812
275.56936
5
−637.38698
17.50000
caf2
6
247.67865
10.07938
7
235.57254
26.31032
caf2
8
3135.07017
78.00000
9
−197.51950
20.09812
caf2
10
−356.26642
10.74741
11
−321.57746
20.31945
caf2
12
−1046.94074
32.68661
13
−269.59967
−32.68661
M1
14
−1046.94074
−20.31945
caf2
15
−321.57746
−10.74741
16
−356.26642
−20.09812
caf2
17
−197.51950
−78.00000
18
3135.07017
−26.31032
caf2
19
235.57254
−10.07938
20
247.67865
−17.50000
caf2
21
−637.38698
−235.06352
22
0.00000
154.78510
FM1
23
412.53248
53.86090
caf2
24
−454.52997
71.16043
25
−247.59332
27.54356
caf2
26
−183.91506
181.23623
27
0.00000
−210.98345
FM2
28
3767.23604
−39.78178
caf2
29
277.50559
−3.63851
30
292.85727
−29.63790
caf2
31
−458.45291
−1.33883
32
−246.79815
−39.85383
caf2
33
−311.59024
−68.58748
34
−235.53718
−52.59735
caf2
35
467.79877
−16.47474
36
245.94544
−23.38703
caf2
37
−2118.42723
−7.42790
38
−493.38965
−20.33655
caf2
39
−516.74517
−17.40457
40
0.00000
7.00000
APERTURE STOP
41
−316.79913
−70.00000
caf2
42
273.85870
−1.51310
43
6275.38113
−69.81106
caf2
44
449.01624
−1.01683
45
−286.22645
−48.61231
caf2
46
−3757.65238
−1.01683
47
−300.84255
−21.04400
caf2
48
−1531.14490
−1.21708
49
−447.05091
−17.57713
caf2
50
−913.33797
−3.39970
51
−417.01084
−21.41824
caf2
52
−42099.53696
−1.01683
53
−233.68723
−47.62945
caf2
54
0.00000
−9.70059
L = 983.40 mm
β = ¼
NA = 0.80
|β1/NAO| = 5.13
|β1 · βf/NAO| = 8.25
|β1| = 1.025
a/b = 0.0455
b/c = 0.518
ASPHERICAL SURFACES
i
K
A
B
C
1
0.49697074
−2.67716672E−09
−1.74309788E−13
−2.09170434E−17
6
1.41328830
2.07799210E−09
−4.26185978E−13
−1.25267670E−17
10
0.46617565
−6.84466829E−09
4.50692462E−14
1.72893414E−18
16
0.46617565
−6.84466829E−09
4.50692462E−14
1.72893414E−18
20
1.41328830
2.07799210E−09
−4.26185978E−13
−1.25267670E−17
23
−1.99692838
−1.46408021E−08
1.07386812E−13
−6.57916448E−18
25
0.94768025
−6.48013865E−09
1.29506074E−13
4.41070720E−18
32
−0.53069421
−2.29496734E−08
1.46540612E−13
−9.48243024E−18
34
−0.58592559
2.27047629E−08
3.72962833E−13
1.78675689E−17
39
−1.99829606
−4.02933770E−08
2.28490744E−13
7.09139430E−18
42
−0.94509911
−1.45135015E−08
7.57078652E−13
−3.77421659E−17
47
−0.10298455
5.88225502E−08
3.64981480E−12
−2.36226284E−16
51
1.94997831
−8.00801793E−08
−2.73886338E−12
1.03434118E−15
53
1.64235579
−5.98172801E−08
1.56058112E−14
−1.19221610E−15
i
D
E
F
G
1
5.18497263E−21
−3.60189028E−25
−2.65126620E−30
8.30507568E−34
6
1.97675878E−21
−4.91077476E−25
3.61319930E−29
−1.06824258E−33
10
9.58499269E−23
1.84965678E−26
−1.35380227E−30
8.38070131E−35
16
9.58499269E−23
1.84965678E−26
−1.35380227E−30
8.38070131E−35
20
1.97675878E−21
−4.91077476E−25
3.61319930E−29
−1.06824258E−33
23
−9.13728385E−22
6.08826931E−26
−1.87726545E−30
−1.11307008E−35
25
1.23647754E−22
5.82476981E−27
−5.35142438E−32
1.80315832E−35
32
−6.38425458E−23
2.33580442E−26
−1.42562786E−30
3.23706771E−35
34
4.66470849E−22
−3.26187824E−26
2.87894208E−30
−1.29130160E−34
39
1.77831564E−22
−9.56219011E−26
2.37030856E−30
−3.53254917E−35
42
1.72360268E−21
−5.67160176E−26
2.05866748E−30
−4.37198713E−35
47
−1.97220610E−20
2.18183279E−24
−1.06203934E−28
3.10574248E−33
51
−8.68250406E−21
2.25723562E−24
3.04027040E−28
−7.08468501E−32
53
−1.80303110E−19
6.84072538E−23
−1.99950230E−26
2.10385493E−30
The first imaging optical system Gr1 includes, in order from the first object 101 side, a lens unit L1A having a positive refractive power, a reciprocating optical system (part) L1B having a negative refractive power, and a concave mirror M1.
The lens unit L1A includes, along the light traveling direction from the side of the first object 101, an positive lens L111 and a positive lens L112. The positive lens L111 has a meniscus form that has a convex surface oriented toward the first object 101 side. The positive lens L112 has an approximately planoconvex form that has a convex surface oriented toward the first object 101 side.
The reciprocating optical system L1B includes an negative lens L113, an aspheric positive lens L114, an aspheric negative lens L115, a negative lens L116, and a concave mirror M1. The negative lens L113 has a meniscus form that has a concave surface oriented toward a side opposite to the first object 101 side. The aspheric positive lens L114 has an approximately planoconvex form that has a convex surface oriented toward the first object 101 side. The aspheric negative lens L115 has a meniscus form that has a concave mirror oriented toward the first object 101 side. The negative lens L116 has a meniscus form that has a concave surface oriented toward the first object 101 side. The concave mirror M1 has a concave form that has a concave surface oriented toward the first object 101 side.
The light from the first object 101 passes through the lens unit L1A, enters the reciprocating optical system L1B, is reflected at the concave mirror M1, and reenters the reciprocating optical system L1B. Then, a deflective reflector FM1 deflects the optical axis AX1 to the optical axis AX2 by 90°. The light is also reflected, and an intermediate image IMG is formed.
The first deflective reflector FM1 is arranged between the first imaging optical system Gr1 and the second imaging optical system Gr2. Preferably, as in the instant embodiment, the first deflective reflector FM1 is arranged between the intermediate image IMG and the reciprocating optical system L1B. In the instant embodiment, the first deflective reflector FM1 uses a flat mirror.
The second imaging optical system Gr2 includes a lens unit L2A having a positive refractive power and a lens unit L2B having a positive refractive power.
The lens unit L2A includes, along the light traveling direction from the side of the first imaging optical system Gr1, an aspheric positive lens L211 and a positive lens L212. The aspheric positive lens L211 has a biconvex form. The positive lens L212 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the intermediate image IMG side.
The lens unit L2B includes a positive lens L213, a negative lens L214, a positive lens L215, an aspheric positive lens L216, a positive lens L217, an aperture stop 103, an aspheric positive lens L218, an aspheric positive lens L219, a positive lens L220, a positive lens L221, an aspheric positive lens L222, a positive lens L223, and an aspheric positive lens L224. The positive lens L213 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The negative lens L214 has a biconcave form. The positive lens L215 has a meniscus form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L216 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The positive lens L217 has a meniscus form that has a convex surface oriented toward the second object 102 side. The aspheric positive lens L218 has a meniscus form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L219 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The positive lens L220 has a meniscus form that has a convex surface oriented toward a side opposite to the second object 102 side. The positive lens L221 has biconvex form. The aspheric positive lens L222 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The positive lens L223 has a meniscus form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L224 has a planoconvex form that has a plane surface oriented toward the second object 102 side.
A space between the final lens (aspheric positive lens L224) and the second object 102 is filled with a fluid (so-called immersion structure).
The second deflective reflector FM2 is arranged between the lens unit L2A and the lens unit L2B of the second imaging optical system Gr2. The present embodiment makes the second deflective reflector FM2 of a plane mirror for deflecting the light reflected from the first deflective reflector FM1 in a predetermined direction.
The aperture stop 103 is arranged between the positive lens L217 and the aspheric positive lens L218.
The catadioptric projection optical system 100 of the fourth embodiment uses a projection magnification of ¼, a reference wavelength of 193.0 nm, and quartz as a glass material. An image-side numerical aperture is NA=0.80. An object-image distance (the first object 101 surface to the second object 102 surface) is L=915.44 mm. An aberration-corrected object point in a range of about 7.50 to 20.25 mm secures a rectangular exposure area of at least 26 mm long and 8 mm wide.
The following Table 4 shows the specification of the numerical example of the catadioptric projection optical system 100 of the first embodiment. Symbols in the table are the same as in table 1, and thus a description thereof will be omitted. A lens glass material SiO2 has a refractive index to a reference wavelength λ=193.000 nm is 1.5609. The refractive indexes of the wavelengths of +0.2 pm and −0.2 pm for the reference wavelength are, 1.56089968 and 1.56090032, respectively. A water used for the fluid has a refractive index to a reference wavelength λ=193.000 nm is 1.437. The refractive indexes of the wavelengths of +0.2 pm and −0.2 pm for the reference wavelength are, 1.43699958 and 1.43700042, respectively.
TABLE 4
DISTANCE FROM FIRST OBJECT~FIRST
SURFACE: 41.84296 mm
LENS
i
ri
di
MATERIAL
1
251.59420
20.22118
sio2
2
243.48822
9.84632
3
358.30042
41.97093
sio2
4
−826.58003
186.17213
5
329.32922
40.00000
sio2
6
143.12035
12.09278
7
185.32312
33.31445
sio2
8
608.10743
78.73433
9
−184.71011
20.00249
sio2
10
−920.52825
18.20389
11
−315.68485
20.04265
sio2
12
−456.66387
47.02968
13
−279.88964
−47.02968
M1
14
−456.66387
−20.04265
sio2
15
−315.68485
−18.20389
16
−920.52825
−20.00249
sio2
17
−184.71011
−78.73433
18
608.10743
−33.31445
sio2
19
185.32312
−12.09278
20
143.12035
−40.00000
sio2
21
329.32922
−172.02999
22
0.00000
188.25827
FM1
23
473.33384
34.33669
sio2
24
−739.09171
1.01738
25
731.11616
48.81832
sio2′
26
−1563.77042
258.82118
27
0.00000
−182.46588
FM2
28
−240.94433
−34.30165
sio2
29
−1065.13094
−26.47287
30
521.68433
−19.11929
sio2
31
−217.81409
−36.69391
32
−197.66602
−26.16167
sio2
33
−301.60112
−73.74535
34
−213.68730
−41.82786
sio2
35
−1000.34292
−59.71802
36
185.13199
−23.38703
sio2
37
192.85517
37.83182
38
0.00000
−39.77435
APERTURE STOP
39
−235.83972
−20.33655
sio2
40
−315.29313
−2.87277
41
−195.62209
−58.03235
sio2
42
942.91191
−8.33243
43
−278.04337
−21.50296
sio2
44
−572.88386
−1.01683
45
−292.77418
−54.84288
sio2
46
1018.86198
−1.01683
47
−507.84505
−20.00707
sio2
48
−2582.58474
−2.79080
49
−249.45727
−23.09053
sio2
50
−604.76780
−1.01683
51
−450.35036
−45.52619
sio2
52
0.00000
−1.19394
Water
L = 915.44 mm
β = ¼
NA = 0.90
|β1/NAO| = 5.16
|β1 · βf/NAO| = 6.90
|β1| = 1.162
a/b = 0.0253
b/c = 0.498
ASPHERICAL SURFACES
i
K
A
B
C
7
0.78454747
−1.25957857E−08
4.07416778E−14
1.60264482E−17
10
−1.69530309
−1.16691839E−08
2.52376221E−13
−1.14340875E−17
16
−1.69530309
−1.16691839E−08
2.52376221E−13
−1.14340875E−17
19
0.78454747
−1.25957857E−08
4.07416778E−14
1.60264482E−17
23
1.91351250
−9.28170033E−09
4.03659464E−14
−1.09106530E−18
34
−0.35639497
1.37284322E−08
1.44579038E−13
1.11740815E−17
40
1.12861801
−3.75383265E−08
−3.76644963E−13
−8.84893402E−18
42
−0.87144860
−1.46351053E−08
5.28358771E−13
−3.55174719E−17
47
−2.01574807
3.61452387E−08
5.16275766E−13
−5.59629177E−16
51
0.25620569
−1.28187111E−07
1.11639829E−11
5.88022359E−15
i
D
E
F
G
7
−8.64081009E−22
2.39680139E−25
−1.80684184E−29
9.97335348E−34
10
3.89781033E−22
8.43163310E−26
−8.08653944E−30
3.19305500E−34
16
3.89781033E−22
8.43163310E−26
−8.08653944E−30
3.19305500E−34
19
−8.64081009E−22
2.39680139E−25
−1.80684184E−29
9.97335348E−34
23
1.57395693E−23
−6.98047575E−28
2.79305776E−32
−5.57070437E−37
34
9.37934698E−23
7.62030685E−27
2.35260178E−32
1.15757755E−35
40
5.33508782E−23
2.65574298E−26
−2.21137735E−30
1.37041063E−34
42
1.34842682E−21
−5.75318986E−26
7.02828620E−31
−2.41667856E−35
47
5.11980199E−20
−3.67799347E−24
2.24192126E−28
−7.90964159E−33
51
−1.38085824E−18
5.33988181E−22
−8.31631159E−26
4.49781606E−30
The first imaging optical system Gr1 includes, in order from the first object 101 side, a lens unit L1A having a positive refractive power, a reciprocating optical system (part) L1B having a negative refractive power, and a concave mirror M1.
The lens unit L1A includes, along the light traveling direction from the side of the first object 101, an positive lens L111 and a negative lens L112. The positive lens L111 has an approximately planoconvex form that has a convex surface oriented toward the first object 101 side. The negative lens L112 has a meniscus form that has a concave surface oriented toward the first object 101 side.
The reciprocating optical system L1B includes a negative lens L113, an aspheric positive lens L114, an aspheric negative lens L115, a positive lens L116, and a concave mirror M1. The negative lens L113 has a meniscus form that has a concave surface oriented toward a side opposite to the first object 101 side. The aspheric positive lens L114 has a meniscus form that has a convex surface oriented toward the first object 101 side. The aspheric negative lens L115 has a meniscus form that has a concave mirror oriented toward the first object 101 side. The positive lens L116 has a meniscus form that has a convex surface oriented toward a side opposite to the first object 101 side. The concave mirror M1 has a concave form that has a concave surface oriented toward the first object 101 side.
The light from the first object 101 passes through the lens unit L1A, enters the reciprocating optical system L1B, is reflected at the concave mirror M1, and reenters the reciprocating optical system L1B. Then, a deflective reflector FM1 deflects the optical axis AX1 to the optical axis AX2 by 90°. The light is also reflected, and an intermediate image IMG is formed.
The first deflective reflector FM1 is arranged between the first imaging optical system Gr1 and the second imaging optical system Gr2. Preferably, as in the instant embodiment, the first deflective reflector FM1 is arranged between the intermediate image IMG and the reciprocating optical system L1B. In the instant embodiment, the first deflective reflector FM1 uses a flat mirror.
The second imaging optical system Gr2 includes a lens unit L2A having a positive refractive power and a lens unit L2B having a positive refractive power.
The lens unit L2A includes, along the light traveling direction from the side of the first imaging optical system Gr1, a positive lens L211, a positive lens L212, and a positive lens L213. The positive lens L211 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the intermediate image IMG side. The positive lens L212 has a biconvex form. The positive lens L213 has an approximately planoconvex form that has a convex surface oriented toward the intermediate image IMG.
The lens unit L2B includes a positive lens L214, an aspheric negative lens L215, an aspheric negative lens L216, a negative lens L217, an aspheric positive lens L218, a positive lens L219, a positive lens L220, a positive lens L221, a positive lens L222, an aperture stop 103, a positive lens L223, an aspheric positive lens L224, an aspheric positive lens L225, an aspheric positive lens L226, and a positive lens L227. The positive lens L214 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric negative lens L215 has an approximately planoconcave form that has a concave surface oriented toward a side opposite to the second object 102 side. The aspheric negative lens L216 has an approximately planoconcave form that has a concave surface oriented toward the second object 102 side. The negative lens L217 has a meniscus form that has a concave surface oriented toward the second object 102 side. The positive lens L218 has a biconvex form. The positive lens L219 has a meniscus form that has a convex surface oriented toward the second object 102 side. The positive lens L220 has a meniscus form that has a convex surface oriented toward the second object 102 side. The positive lens L221 has a meniscus form that has a convex surface oriented toward a side opposite to the second object 102 side. The positive lens L222 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The positive lens L223 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L224 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L225 has a planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The aspheric positive lens L226 has an approximately planoconvex form that has a convex surface oriented toward a side opposite to the second object 102 side. The positive lens L227 has a planoconvex form that has a plane surface oriented toward the second object 102.
A space between the final lens (positive lens L227) and the second object 102 is filled with a fluid (so-called immersion structure).
The second deflective reflector FM2 is arranged between the lens unit L2A and the lens unit L2B of the second imaging optical system Gr2. The present embodiment makes the second deflective reflector FM2 of a plane mirror for deflecting the light reflected from the first deflective reflector FM1 in a predetermined direction.
The aperture stop 103 is arranged between the positive lens L222 and the positive lens L223.
The catadioptric projection optical system 100 of the fifth embodiment uses a projection magnification of ¼, a reference wavelength of 193.0 nm, and quartz as a glass material. An image-side numerical aperture is NA=0.80. An object-image distance (the first object 101 surface to the second object 102 surface) is L=1166.42 mm. An aberration-corrected object point in a range of about 11.25 to 17.00 mm secures a rectangular exposure area of at least 21 mm long and 4 mm wide.
The following Table 5 shows the specification of the numerical example of the catadioptric projection optical system 100 of the fifth embodiment. Symbols in the table are the same as in table 1, and thus a description thereof will be omitted.
TABLE 5
DISTANCE FROM FIRST OBJECT~FIRST
SURFACE: 20.37598 mm
LENS
i
ri
di
MATERIAL
1
203.00558
20.22118
sio2
2
576.42020
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sio2
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sio2
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M1
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201.39136
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sio2
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400.38641
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0.00000
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FM1
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sio2
24
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1547.35845
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sio2
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574.67919
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sio2
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0.00000
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FM2
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sio2
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sio2
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1225.43863
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0.00000
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APERTURE STOP
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sio2
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0.00000
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Water
L = 1166.42 mm
β = ¼
NA = 1.20
|β1/NAO| = 4.01
|β1 · βf/NAO| = 10.51
|β1| = 1.203
a/b = 0.104
b/c = 0.577
ASPHERICAL SURFACES
i
K
A
B
C
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i
D
E
F
G
7
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10
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The catadioptric projection optical system of the present invention reduces the incident angle and the incident angle range of light upon the deflective reflectors (optical path deflective mirror)and can easily control reflection film properties. Moreover, the catadioptric projection optical system of the present invention can obtain a large enough imaging area width with no light shielding at the pupil, and stably achieve the superior imaging performance. Especially, the influence to the imaging performance by reflection film properties that raises a problem at higher NA can be controlled. Moreover, the catadioptric projection optical system of the present invention avoids the interference between the light and the lens, reduces the incident angle range on the plane mirror, thus, achieves easiness of the control of reflection film properties. Additionally, the catadioptric projection optical system of the present invention controls the generation of chromatic coma aberration.
Referring now to
The exposure apparatus 200 is an immersion type exposure apparatus that exposes onto an object 240 a circuit pattern of a reticle 220 via a fluid WT supplied between a final lens surface at the object 240 side of a projection optical system 100 and the object 240 in a step-and-scan manner or step-and-repeat manner. Such an exposure apparatus is suitable for a sub-micron or quarter-micron lithography process. The instant embodiment exemplarily describes a step-and-scan exposure apparatus (which is also called “scanner”). “The step-and-scan manner”, as is used herein, is an exposure method that exposes a reticle pattern onto a wafer by continuously scanning the wafer relative to the reticle, and by moving, after a shot of exposure, the wafer stepwise to the next exposure area to be shot. “The step-and-repeat manner” is another mode of exposure method that moves a wafer stepwise to an exposure area for the next shot every short of cell projection.
The exposure apparatus 200 includes, as shown in
The illumination apparatus 210 illuminates the reticle 220 that forms the circuit pattern to be transferred, and includes a light source unit 212 and the illumination optical system 214.
The light source unit 212, as an example, uses a light source such as ArF excimer laser with a wavelength of approximately 193 [nm] and KrF excimer laser with a wavelength of approximately 248 [nm]. However, the laser type is not limited to excimer lasers because for example, F2 laser with a wavelength of approximately 157 [nm] and a YAG laser may be used. Similarly, the number of laser units is not limited. For example, two independently acting solid lasers would cause no coherence between these solid lasers and significantly reduces speckles resulting from the coherence. An optical system for reducing speckles may swing linearly or rotationally. A light source applicable for the light source unit 212 is not limited to a laser, and may use one or more lamps such as a mercury lamp and a xenon lamp.
The illumination optical system 214 is an optical system that illuminates the reticle 220, and includes a lens, a mirror, an optical integrator, a stop, and the like, for example, a condenser lens, an optical integrator, an aperture stop, a condenser lens, a slit, and an image-forming optical system in this order. The illumination optical system 214 can use any light regardless of whether it is on-axial or off-axial light. The optical integrator may include a fly-eye lens or an integrator formed by stacking two sets of cylindrical lens array plates (or lenticular lenses), and be replaced with an optical rod or a diffractive element.
The reticle 220 is, for example, reflection or penetration reticle, and forms the circuit pattern to be transferred. The reticle 220 is supported and driven by the reticle stage 230. Diffracted light emitted from the reticle 220 passes the catadioptric projection optical system 230 and is then projected onto the plate 540. The reticle 220 and the object 240 are located in an optically conjugate relationship. Since the exposure apparatus 200 of the instant embodiment is a scanner, the reticle 220 and the object 240 are scanned at the speed of the reduction ratio. Thus, the pattern on the reticle 220 is transferred to the object 240. If it is a step-and-repeat exposure apparatus (referred to as a “stepper”), the reticle 220 and the object 240 remain still in exposing the reticle pattern.
The reticle stage 230 supports the reticle 220 via a reticle chuck (not shown), and is connected to a moving mechanism (not shown). The moving mechanism includes a linear motor, etc., and moves the reticle 220 by driving the reticle stage 230 at least in a direction X. The exposure apparatus 200 scans the reticle 220 and the object 240 synchronously by the controller (not shown). Here, X is a scan direction on the reticle 220 or the object 240, Y is a direction perpendicular to it, and Z is a perpendicular direction to the surface of reticle 220 or the object 240.
The catadioptric projection optical system 100 is a catadioptric projection optical system that projects the pattern on the reticle 220 onto the image surface. The catadioptric projection optical system 100 can apply any embodiments as above-mentioned, and a detailed description will be omitted.
The object 240 is, in the instant embodiment, a wafer, which includes a glass plate for the liquid crystal substrate and other objects. Photoresist is applied to the object 240.
The wafer stage 250 supports the object 240 via a wafer chuck (not shown). The wafer stage 250 moves the object 250 in X-Y-Z directions by using a linear motor similar to the reticle stage 230. The positions of the reticle stage 230 and wafer stage 250 are monitored, for example, by a laser interferometer and the like, so that both are driven at a constant speed ratio. The wafer stage 250 is installed on a stage stool supported on the floor and the like, for example, via a dumper, and the reticle stage 230 and the catadioptric projection optical system 100 are installed on a lens barrel stool (not shown) supported, for example, via a dumper to the base frame placed on the floor.
The fluid supply-recovery mechanism 260 supplies the fluid WT between the catadioptric projection optical system 100 and the object 240, which in detail means between the final lens surface at the object 240 side of the catadioptric projection optical system 100 (optical element arranged on the object 240 side final edge of the catadioptric projection optical system 100) and recovers the supplied fluid WT. In other words, the space formed on the catadioptric projection optical system 100 and the surface of the object 240 is filled with the fluid WT supplied from the fluid supply-recovery mechanism 260. The fluid WT is, in the instant embodiment, pure water. However, the fluid WT is not limited to pure water, can use a fluid that has high transmittance property and refractive index property for a wavelength of the exposure light, and high chemical stability to the catadioptric projection optical system 100 and the photoresist spread on the object 240. For example, fluorine system inert fluid may be used.
The controller (not shown) includes a CPU and memory (not shown) and controls operation of the exposure apparatus 200. The controller is electrically connected to the illumination apparatus 210, (the moving mechanism (not shown) for) the reticle stage 230, (the moving mechanism (not shown) for) the wafer stage 250, and the fluid supply-recovery mechanism 260. The controller controls the supply and recover of the fluid WT, switch of stop, and supply and recover amount of the fluid WT based on a condition such as a drive direction of the wafer stage 250 during the exposure. The CPU includes a processor regardless of its name, such as an MPU, and controls each module. The memory includes a ROM and RAM, and stores a firmware for controlling the operations of the exposure apparatus 200.
In exposure, light is emitted from the light source unit 212, e.g., Koehler-illuminated the reticle 220 via the illumination optical system 214. Light that passes through the reticle 220 and reflects the reticle pattern is imaged onto the object 240 by the catadioptric projection optical system 100. The catadioptric projection optical system 100 used for the exposure apparatus 200 has a superior imaging performance, and can provide devices, such as semiconductor chips, such as LSIs and VLSIs, CCDs, LCDs, magnetic sensors, and thin-film magnetic heads, with high throughput and economic efficiency.
Referring now to
Furthermore, the present invention is not limited to these preferred embodiments and various variations and modifications may be made without departing from the scope of the present invention. For example, the present invention can be applied to an exposure apparatus other than the immersion exposure apparatus.
This application claims a foreign priority benefit based on Japanese Patent Application No. 2004-309129, filed on Oct. 25, 2004, which is hereby incorporated by reference herein in its entirety as if fully set forth herein.
Terasawa, Chiaki, Morishima, Hideki, Katashiba, Yuji
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| Oct 14 2005 | MORISHIMA, HIDEKI | Canon Kabushiki Kaisha | ASSIGNMENT OF ASSIGNORS INTEREST SEE DOCUMENT FOR DETAILS | 017148 | /0320 | |
| Oct 15 2005 | KATASHIBA, YUJI | Canon Kabushiki Kaisha | ASSIGNMENT OF ASSIGNORS INTEREST SEE DOCUMENT FOR DETAILS | 017148 | /0320 | |
| Oct 15 2005 | TERESAWA, CHIAKI | Canon Kabushiki Kaisha | ASSIGNMENT OF ASSIGNORS INTEREST SEE DOCUMENT FOR DETAILS | 017148 | /0320 | |
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| Apr 26 2016 | Micron Technology, Inc | U S BANK NATIONAL ASSOCIATION, AS COLLATERAL AGENT | CORRECTIVE ASSIGNMENT TO CORRECT THE REPLACE ERRONEOUSLY FILED PATENT #7358718 WITH THE CORRECT PATENT #7358178 PREVIOUSLY RECORDED ON REEL 038669 FRAME 0001 ASSIGNOR S HEREBY CONFIRMS THE SECURITY INTEREST | 043079 | /0001 |
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